Method and apparatus for performing signal correlation

ABSTRACT

A method of computing a correlation between a pseudorandom reference code and a satellite signal is provided. The method comprises receiving a satellite signal having a repeating code modulated thereon, wherein the satellite signal comprises a pseudorange; correlating the satellite signal with less than an entire length of the pseudorandom reference code with a portion of the satellite signal to produce a correlation over a period less than a period of the repeating code; and processing the correlation to form values representative of magnitude or power of the correlation to produce an energy signal.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation of U.S. patent application Ser. No. 10/394,404, filed Mar. 21, 2003, now U.S. Pat. No. 7,190,712 which is a continuation-in-part of U.S. patent application Ser. No. 09/900,499, filed Jul. 6, 2001 (now U.S. Pat. No. 6,704,348, issued Mar. 9, 2004), which is a continuation-in-part of U.S. patent application Ser. No. 09/861,086, filed May 18, 2001 (now U.S. Pat. No. 6,606,346, issued Aug. 12, 2003), each of which are incorporated herein by reference in their entireties.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to signal correlators for digital signal receivers and, more particularly, the invention relates to a method and apparatus for performing signal correlation in, for example, a global positioning system (GPS) receiver.

2. Description of the Related Art

The process of measuring a global positioning system (GPS) signal begins with a procedure to search for the GPS signal in the presence of noise by attempting a series of correlations of the incoming signal against a known pseudo-random noise (PRN) code. The search process can be lengthy, as both the exact frequency of the signal and the time-of-arrival delay are unknown; To find the signal, receivers traditionally conduct a two dimensional search, checking each delay possibility at every possible frequency. To test for the presence of a signal at a particular frequency and delay, the receiver is tuned to the frequency, and the incoming signal is correlated with the known PRN code delayed by an amount corresponding to the time of arrival. If no signal is detected, the search continues to the next delay possibility, and after all delay possibilities are checked, continues to the next frequency possibility. Each individual correlation is performed over one or more milliseconds in order to allow sufficient signal averaging to distinguish the signal from the noise. Because many thousand frequency and delay possibilities are checked, the overall acquisition process can take tens of seconds.

Recently, new applications of GPS technology in wireless devices have emerged, for example, the use of GPS in cellular phones to provide emergency location capability. In these applications, rapid signal acquisition in just a few seconds is required. Furthermore, these applications require a GPS receiver to operate in harsh signal environments and indoors, where GPS signal levels are greatly attenuated. Detecting attenuated signals requires each correlation to be performed over a relatively long period of time. For example integration may be performed over a few seconds, as opposed to the 1-10 millisecond period used in traditional GPS receivers. The two dimensional sequential search process employed by traditional receivers becomes impractical at such long integration times, because the overall search time increases by a factor of 100 or more.

To accelerate the search process, GPS designers add additional correlators to the receiver so that multiple time of arrival possibilities can be checked simultaneously. Typically, each correlator that is added requires a separate code mixer and signal accumulator. For a given sensitivity level, this decreases search times in proportion to the number of correlators. To achieve the sensitivity and acquisition time demanded in cellular phone applications, the design might have to incorporate thousands of correlators. This addition is typically prohibitively complex and expensive for a consumer class device.

For example, U.S. Pat. No. 5,901,171, issued May 4, 1999, describes a triple multiplexing technique that allows a single time shared processing block to be used to perform up to 20 simultaneous correlations on each of 12 channels. This offers an improvement in performance relative to single correlator designs since blocks of 20 delay possibilities are checked simultaneously. A full signal search over a full range of delay uncertainties requires using the block of 20 correlators approximately 100 times in succession to check 2046 delays. Thus, if an acquisition must be performed in a few seconds, the integration time is limited to tens of milliseconds. This is insufficient to achieve the sensitivity needed for indoor GPS applications.

To further improve the search process, other GPS receiver architectures include processing capable of generating a convolution between the incoming signal and the known PRN code. This is equivalent to providing a complete set of correlators spanning all time delay possibilities over a full C/A code epoch (1023 chips), and U.S. Pat. No. 5,663,734, issued Sep. 2, 1997, describe fast Fourier transform (FFT) based software techniques to efficiently generate the necessary correlation results using software algorithms. This approach is not suitable for all applications, because a programmable digital signal processor (DSP) is needed to run the software FFT, and a large memory is needed to store unprocessed signal samples. Furthermore, this approach can have a large processing delay due to the software computations and the fact that software processing starts only after a complete snapshot of the signal is stored. In many applications, a real time processing solution is preferred, preferably one that does not involve extensive software processing. Lyusin et al., “Fast Acquisition by Matched Filter Technique for GPS/GLONASS Receivers”, pp 307-315 describes hardware approaches to performing the convolution in real time using a matched filter with 1023 taps. The matched filter consists of shift registers large enough to hold a full C/A code epoch, as well as a width 1023 vector multiplier and adder unit that generates the inner product between a full epoch of the signal and the C/A code.

This circuit is complex relative to the constraints of low cost consumer devices such as cellular phones. Other matched filter approaches, such as utilized in military class receivers for P-code acquisition, also incorporate large vector multipliers.

Thus, there is a need for an improved, simple and low cost GPS processing block capable of processing an entire epoch of signal and C/A code. Such a device must be built from hardware of relative simplicity, yet be capable of generating a full convolution, or many parallel correlations, preferably without a large vector multiplier.

SUMMARY OF THE INVENTION

The invention provides a method and apparatus for computing a full convolution between an input signal (e.g., a GPS signal) and a pseudorandom noise (PRN) code reference by generating the convolution result in real time without storing unprocessed signal samples, and without extensive software processing. The apparatus comprises a vector multiplier running at high speed to achieve the same result as a vector multiplier sized to process an entire epoch. The invention can be implemented in an integrated circuit that fits the complexity constraints of a consumer class device such as a cellular phone. The design includes the necessary logic to enable long term averaging of convolution results to ensure high sensitivity. This invention is capable of correlating signals for use in deriving a position location from highly attenuated signals, including signals received indoors.

The complete apparatus consists of a conventional GPS tuner, a decimation circuit, a convolution processor, and RAM blocks that accumulate convolution results. The convolution processor runs at a high clock rate on the order of 100 MHz and higher enabling the computation of a full convolution by repeated use of a small block of circuitry. Specifically, each point of the convolution is decomposed into a series of partial correlations, each of which is generated using a vector multiplier that is sized to process only a portion of an epoch. The apparatus organizes the partial correlations by subdividing the C/A code into a non-overlapping set of code segments. Each partial correlation uses only one code segment at a time, allowing the C/A code to be stored and retrieved efficiently, using a simple lookup table.

The processor begins by decimating input IF samples to create a signal stream at a desired sample rate, where the rate is precisely matched to the timing of the incoming signal. If the desired sample rate is Pf_(o) (P samples per C/A chip) then the sampling rate is set so that exactly 1023×P samples are taken in each signal epoch. The processor correlates the signal clocking signals through shift registers sized to hold P×K input samples, where K is a factor of 1023. At each signal shift, a series of M partial correlation operations are performed with M chosen such that M×K=1023. Each partial correlation consists of taking the inner product of the contents of the signal shift registers with a block of reference samples created by extending a length K segment of the C/A code to P×K samples. Partial correlation results are accumulated in memory. By accumulating partial correlation results, the processor generates complete correlation results for many correlation points, up to the full convolution.

In an alternative embodiment, the invention provides for two modes of operation. In a standard mode of operation, a full convolution is generated using a standard chip spacing, typically ½ a C/A code chip. In a high-resolution mode, a portion of the convolution is generated using a reduced chip spacing, for example, ⅕ of a C/A code chip. The transition between modes is controlled by algorithms and occurs when previous measurements and/or externally available information focus the acquisition in a portion of the convolution in which high-resolution correlations are computed.

In another embodiment, a method of computing a correlation between a digital signal having a repeating code and a pseudorandom reference code using a sub-epoch coherent integration period is described. Portions of a pseudorandom reference code are multiplied with portions of the repeating code of the digital signal to produce a plurality of inner products. The plurality of inner products are then integrated over a period less than a period of the repeating code to produce a correlation result with a broadened frequency response. In an embodiment, values representative of magnitude or power of the partial correlation are formed to produce an energy signal. Multiple energy signals are produced in a similar fashion and are summed over a predetermined period.

In yet another embodiment, a method of estimating a frequency shift in a digital signal having a repeating code is described. The digital signal is correlated with a pseudorandom reference code to produce a first correlation. The digital signal is then correlated with the pseudorandom reference code to produce a second correlation. The first and second correlations are then used to determine first and second signal delays. The frequency shift of the digital signal is computed using a difference between the first and second signal delays over time. In an embodiment, the first and second correlations are produced using a first coherent integration period. Then, at least one additional correlation is performed using a second coherent integration period that is longer than the first coherent integration period. In one example, the first coherent integration period may be less than a period of the repeating code.

In another embodiment, a method of computing a correlation between a pseudorandom reference code and a satellite signal comprises receiving a satellite signal having a repeating code modulated thereon, wherein the satellite signal comprises a pseudorange; correlating the satellite signal with less than an entire length of the pseudorandom reference code with a portion of the satellite signal to produce a correlation over a period less than a period of the repeating code; and processing the correlation to form values representative of magnitude or power of the correlation to produce an energy signal.

BRIEF DESCRIPTION OF THE DRAWINGS

So that the manner in which the above recited features of the present invention are attained and can be understood in detail, a more particular description of the invention, briefly summarized above, may be had by reference to the embodiments thereof which are illustrated in the appended drawings.

It is to be noted, however, that the appended drawings illustrate only typical embodiments of this invention and are therefore not to be considered limiting of its scope, for the invention may admit to other equally effective embodiments.

FIG. 1 shows a block diagram of a GPS receiver comprising the present invention;

FIG. 2 shows an example of waveforms produced by the invention of FIG. 1;

FIG. 3 shows details of an accumulated magnitude waveform of FIG. 2;

FIG. 4 shows a detailed block diagram of one embodiment of the convolution processor and the convolution results processing circuits;

FIG. 5 depicts a flow diagram of a method of operation of the invention of FIG. 1;

FIG. 6 graphically illustrates a simplified example of computing a full convolution in the traditional manner;

FIG. 7 graphically illustrates how the full convolution of FIG. 6 is performed using the invention;

FIG. 8 illustrates an embodiment of a code lookup apparatus suitable for use in the invention of FIG. 1;

FIG. 9 illustrates an embodiment of a two-dimensional code shift register suitable for use in an alternate embodiment of the invention of FIG. 1;

FIG. 10 shows a block diagram of a GPS receiver comprising an alternative embodiment of the invention;

FIG. 11 shows details of an accumulated magnitude waveform in high resolution mode;

FIG. 12 illustrates an embodiment of a code lookup apparatus suitable for use in the invention of FIG. 10; and

FIG. 13 depicts a flow diagram of a method of operation of the invention of FIG. 10;

FIG. 14 depicts a graph showing exemplary frequency response waveforms for various coherent integration periods in accordance with one or more aspects of the invention;

FIG. 15 depicts a graph showing exemplary frequency response waveforms for different frequency bins in accordance with one or more aspects of the invention; and

FIG. 16 depicts a flow diagram showing an embodiment of a process for estimating the frequency error in the received signals in accordance with one or more aspects of the invention.

DETAILED DESCRIPTION OF THE INVENTION

FIG. 1 depicts a block diagram of a global positioning system (GPS) receiver 100 incorporating the present invention. The use of a GPS receiver as the platform within which the invention is incorporated forms one application of the invention. Other platforms that require signal correlation may find use for the present invention.

Signals (such as GPS signals) are received by an antenna 101. A radio-frequency-to-intermediate-frequency converter (RF/IF converter) 102 filters, amplifies, and frequency shifts the signal for digitization by an analog-to-digital converter (A/D) 103. The elements 101, 102 and 103 are substantially similar to those elements used in a conventional GPS receiver.

The output of the A/D 103 is coupled to a set of processing channels 104 ₁, 104 ₂, . . . 104 _(n) (where n is an integer) implemented in digital logic. Each processing channel 104 _(n) may be used to process the signal from a particular GPS satellite. The signal in a particular channel is tuned digitally by a tuner 105, driven by a numerically controlled oscillator (NCO) 106. The tuner 105 serves two purposes. First, the IF frequency component remaining after RF/IF conversion is removed. Second, the satellite Doppler frequency shift resulting from satellite motion, user motion, and reference frequency errors is removed. The output from the tuner is a baseband signal consisting of an in-phase component (I) and a quadrature component (Q). The tuner 105 and Carrier NCO 106 are substantially similar to those used in conventional GPS receiver designs.

A decimation circuit 107 processes the output of the tuner 105. The output of the decimation circuit 107 is a series of complex signal samples with I and Q components, output at a rate precisely timed to match the timing of the input signal. In one embodiment of the invention, the decimation operation is a simple pre-summer that sums all the incoming signal samples over the period of an output sample. A numerically controlled oscillator (NCO) 108 is used to time the sampling process. For example, if P=2, the code NCO 108 is set to generate a frequency of (2×f_(s)), where f_(s) is f_(o) (the GPS signal's C/A code chipping rate), adjusted for Doppler shift. The NCO adjusts for Doppler shift based on external input from firmware commands. Because the Doppler shift is different for each satellite, a separate code NCO 108 and decimation circuit 107 is required for each channel 104 _(n). It should be noted that there is no requirement that the incoming sample rate be an integer multiple of the f_(s), as the code NCO 108 is capable of generating an arbitrary frequency. If the decimation circuit 107 is a pre-summer, the number of samples summed will typically toggle between two values, so that over the long term, the correct sample timing is maintained. For example, if the incoming sample rate is 10 MHz, and the desired sample rate is 2.046 MHz, the pre-summer will add either 4 or 5 samples, so that the desired sample rate is maintained on average.

The decimation circuit 107 may also include a quantizer (not shown) at its output to reduce the number of bits in the signal components before further processing. In one embodiment of the invention, 2-bit quantization is used.

The signal samples from decimation circuit 107 are coupled to a convolution processor 109. The convolution processor 109 generates results that are stored in signal random access memories (RAMs) 110 a and 110 b. Specifically, these RAMs 110 a and 110 b hold a complex vector that makes up all or part of the full convolution between the input signal and a reference PN code (e.g. a GPS C/A code). The convolution result will have a peak at points corresponding to high correlation between the signal and reference (the PN code). As shall be discussed in detail below, the relative location of these peaks for various satellite signals is used to ultimately compute position information.

The convolution processor 109 and signal RAMs 110 a and 110 b accumulate convolution results for multiple epochs of the GPS signal, which repeats at nominal 1 millisecond intervals. For example, if 10 milliseconds of the signal are processed, the values in RAM 110 a and 110 b are the sum of 10 correlation results each generated over one epoch. All the individual correlations should have a similar characteristic, since the timing of the decimation operation ensures that samples are taken at the same relative moment within each epoch. Accumulating similar results from individual correlations improves the signal to noise ratio, enhancing the ability of the receiver to detect weak signals. This processing may be referred to as coherent integration and, as will be discussed, can be combined with magnitude integration to yield correlation results averaged over a time period of up to several seconds.

The length of time over which coherent integration interval is performed is limited by several factors, including uncompensated Doppler shift, GPS signal navigation data bits, and phase shifts induced by motion of the receiver 100. These factors introduce slow, but seemingly random phase variations into the signals. Over many tens of milliseconds, these phase changes cause destructive interference that defeats the purpose of coherent integration. Therefore, to achieve long averaging intervals, the receiver 100 performs a secondary step of magnitude accumulation. Specifically, the signals stored in the signal RAMs 110 a and 110 b are periodically output to a complex normalizer 111 that generates a complex magnitude value of the complex convolution vector. The complex magnitude values are accumulated by an adder 112 and stored in magnitude RAM 113. Each time the complex magnitude of the signal is computed, the signal RAMs 110 a and 110 b are cleared to allow another coherent integration to occur. The process continues until the desired number of magnitude accumulations is completed. For example, if the coherent averaging interval is 10 milliseconds, and 200 magnitude accumulations are desired, the total process will run over 2 seconds.

After convolution processing, the magnitude RAM 113 contains a vector containing the complex magnitude of the convolution result, integrated to improve signal-to-noise ratio. As shall be discussed below, this vector is further processed by software algorithms that are executed by the CPU 114 to produce pseudorange data that is used to yield the position of the receiver. It should be noted that the CPU computational load for these steps is quite modest compared to a conventional GPS receiver or an FFT based correlator. In this implementation, the computationally intensive tasks of correlation and integration are completed prior to software processing.

FIG. 2 depicts waveforms 201I, 201Q and 202 generated by the components of FIG. 1. The waveforms 201I, 201Q and 202 are plots of signal strength (axis 208) versus code chips (axis 210). The waveforms depict the output of the convolution processor 109 during coherent integration and magnitude integration. For clarity, only 9 milliseconds of signal processing time is shown consisting of 3 magnitude accumulations each based on 3 coherent integrations. In the example, P=2, so there are 2046 signal samples per coherent integration. Waveforms 201I and 201Q are the output from the convolution processor 109 where 201I is the I-component of the output and 201Q is the Q-component. Each block of 2046 samples is a full convolution result, generated in real time by the convolution processor 109 from the 2046 signal samples processed during the interval. The convolution result contains noise except in the vicinity of a single peak (such as indicated by reference numbers 206I and 206Q) corresponding to the time delay of the signal. The signal repeats every epoch, so the peak reappears each 2046 samples. Over the first three cycles, correlation results are accumulated in the RAM 110 a and 110 b by summing values at corresponding delays from each epoch. (For example, the values at output time 4 are summed with the values at output time 2050 and 4096.) The correlation peak always appears at the same delay offset and the size of the peak increases over the accumulation, roughly tripling over 3 epochs. The level of the noise also increases, but rises only as the square root of 3 because the noise correlation is uncorrelated from epoch to epoch. The signal to noise ratio improves through the accumulation process, increasing by roughly the square root of 3. Waveform 201Q illustrates the same signal accumulation process occurring in the quadrature channel.

Beginning with the 4^(th) cycle of the signal, the signal RAMs 110 a and 110 b are cleared to zero, and the signal accumulation process begins again. Waveforms 201I and 201Q show the correlations accumulating and dumping 3 times over 9 signal epochs.

At the end of the coherent averaging interval the accumulated signal's magnitude is computed and summed into the magnitude RAM 113. The signal in the magnitude RAM 113 is shown as waveform 202. In the example, the waveform 202 updates three times corresponding to the completion of each coherent integration. The peaks are identified by reference numbers 212 ₁, 212 ₂, 212 ₃ and noise is identified by reference number 214. As can be seen, the signal-to-noise ratio increases with each magnitude accumulation, further enhancing the ability of the system to identify the peak corresponding to the time of arrival.

It should be noted that in the example, the complex phase of the signal varied over the 9 epochs. In particular, the signal was initially present in both I and Q channels, but by the final epoch, had rotated so that the signal was strong in the I channel and nearly absent in the Q channel. As mentioned above, imperfect Doppler shift tuning and other effects cause this rotation. Over many epochs, the phase would rotate through many cycles, resulting in cancellation of the signal when accumulated. For this reason, the inventive receiver accumulates coherently over only a short interval, relying on magnitude (non-coherent) accumulation for long term averaging. Magnitude values are independent of phase, and may be successfully integrated over several seconds.

FIG. 3 illustrates the accumulated magnitude waveform 202 in greater detail. The plot 300 shows the magnitude of the convolution in the vicinity of a peak 212 ₃ corresponding to the time delay of the signal. Points on the code chip axis 210 are spaced at an interval equal to the C/A code chip length divided by P, where P is the ratio of the signal sampling rate to f_(o), the C/A code chipping rate. In the example, P=2, so the points are spaced at ½ chip intervals, or approximately 500 ns. (This spacing in time corresponds to a range difference of 150 meters). In order to achieve pseudorange measurements on the order of ten meters or better, the convolution results are further processed, typically in the CPU 114, to produce the position information. There are numerous interpolation techniques that can be used to estimate the true time delay, using the discrete correlation values provided by the convolution process. One embodiment uses a least squares estimation technique to identify parameters of a signal that best fits the noisy measured data. The ideal response of a signal is the magnitude of the autocorrelation of the signal. This waveform can easily be shown to have the form of a raised triangle 302. The width 303 of the triangle base is exactly 2 C/A code chips, or 4 points on the convolution result (for the P=2 case). The height 304 of the base of the triangle is the magnitude of the noise in the convolution for time delays not corresponding to the signal. The magnitude of this noise can be estimated from the data or pre-calculated based on design parameters, such as the amplifier noise figure, cable and filter loss and system temperature. The peak 305 of the triangle and the center 306 of the triangle are unknowns corresponding to the signal magnitude and time delay. The least squares method can be used to estimate these two parameters so as to fit the noisy data points to a triangle with a given peak and center.

FIG. 4 depicts a detailed block diagram of the convolution processor 109 (as well as the convolution results processing circuits 400), in particular details showing how a full convolution is generated by repeated use of a small block of circuitry. Operation of the circuits in this embodiment can be best understood with simultaneous reference to FIG. 4, a flow diagram of FIG. 5 representing the operation of the processor 109 of FIG. 4, and by comparison of the simple examples of FIG. 6 and FIG. 7.

Signals from the decimation circuit 107 are coupled to shift registers 401 a and 401 b, handling I and Q components, respectively. Each shift register 401 a and 401 b is of length P×K, where P is the desired number of samples per C/A code chip, and K is chosen as a design parameter. As will be explained K is a factor of 1023. To simplify the discussion, the remainder of the discussion focuses on one particular embodiment with P=2 (samples spaced ½ chip apart) and K=33. This means of advancing the signal through the shift register eliminates the need for circuitry to double-buffer the signal, reducing the cost and complexity of implementation.

Signals advance through shift registers 401 a and 401 b at the rate of 2f_(o), as timed by the code NCO 108. The signals remain in place in the shift registers for many clock cycles, so that a series of partial correlation operations can be performed. Specifically, a total of M partial correlations are performed, where M=1023/K or 31 in this example. Each partial correlation consists of a fast vector multiply and add operation between the contents of each signal shift register and a segment of the code containing P×K (e.g., 66) code samples. The fast vector multiplication and addition occurs in circuits 402 a and 402 b. Circuits 402 a and 402 b respectively comprise multipliers 410 a and 410 b and summers 412 a and 412 b. The operation consists of multiplying each of the 66 signal samples in the signal register 401 a or 401 b by 66 code samples (formed by extending 33 code samples with the code extender 409), and summing the results in summer 412 a and 412 b. The operation occurs separately and simultaneously in the I and Q channels. Mathematically, this operation is referred to as an inner product, defined as

$\sum\limits_{i = 1}^{P \times K}{\text{<}{signal}_{i}\text{>}\;\text{<}{code}\mspace{14mu} c_{i}\text{>}}$ The output of the vector multiply and add may be re-quantized to keep the numbers in a small range so as to avoid overflowing RAMs 404 a and 404 b. For simplicity, the quantizer is not shown. In one embodiment, the re-quantization is to 2 bits of resolution.

The results of the vector multiply and add are accumulated by adders 403 a and 403 b and processed by the convolution results processing circuits 400. Circuits 400 comprise signal RAM 110 a, 110 b, complex normalizer 111, adder 112 and magnitude RAM 113. The accumulation process consists of reading from RAM 110 a and 110 b the current values for a particular time delay, adding the just computed partial correlations, and writing the sums back to RAMs 110 a and 110 b . By properly combining partial correlations that correspond to a particular time delay, the full correlation for that delay is computed. As described previously, the process continues for as many epochs of the signal as desired to enhance signal to noise ratio. Thus, the adders 403 a and 403 b serve two purposes: the combining of partial correlations within an epoch; and the accumulation of correlations across several epochs.

The outputs from signal RAMs 110 a and 110 b are combined in complex normalizer 405 to form the magnitude of the signal. The I and Q waveforms in these RAMs 110 a and 110 b can be viewed as the real and imaginary part of a complex waveform. Forming the magnitude consists of squaring each component, summing the results, and taking the square root of the result. There are several approximations to the magnitude that can be used to simplify circuitry. In one embodiment, the complex magnitude is approximated by taking the scalar magnitude of I and Q independently and determining which is larger. The magnitude can be approximated by taking the larger magnitude and adding it to the one half of the smaller magnitude.

The results of the magnitude operation may be scaled to keep the values in a small range so as to avoid overflowing RAM 113. For simplicity, a scaler is not shown. In one embodiment, the scaling consists of shifting the result by 3 bits (i.e., divide by 8).

It would also be possible to accumulate signal powers rather than signal magnitudes. In this case, the operation in 405 would be power estimation, typically computed by taking the sum of the squares of I and Q. In this case, the pseudorange determination algorithms described in reference to FIG. 3 would have to be slightly modified to perform a fit against a power waveform as opposed to a magnitude waveform. Alternatively, additional nonlinear operations could be used to generate values representative of the magnitude or power of I and Q.

The output from complex normalizer 111 is accumulated by the adder 112 into magnitude RAM 113. The accumulation process consists of reading from RAM 113 the current magnitude value for a particular time delay, adding in the just computed magnitude result, and writing the sum back to the RAM 113. As discussed previously, the magnitude accumulation continues for as many cycles as required to achieve signal to noise ratio enhancement.

The vector multipliers 402 a and 402 b perform M partial correlations for each shift of the signal. A code lookup circuit 408 generates the reference code samples for each partial correlation. The lookup is controlled by two lookup indexes. First, the code must be selected from 1 of 32 codes. This selection is constant through the convolution process and is established when the processing channel is configured to correlate for a particular satellite signal. The second index is a segment index between 1 and M. Each C/A code consists of 1023 chips, which are divided into M non-overlapping segments each consisting of K adjacent code chips. The lookup index identifies which code segment is needed. The output from the code lookup circuit is K chips comprising the segment. The selection process is controlled by Control/Address Logic 414.

The code extender 409 takes as its input K chips of a segment and extends the segment into K×P code samples. The extension operation consists of converting each code chip into P identical code samples. The output from the code extender 409 forms the reference code input to vector multipliers 402 a-b. In the example, the output from the code extender is 66 samples made up of 33 unique values, each replicated twice.

The architecture shown in FIG. 4 requires a clock that is substantially faster than the C/A code rate f_(o). For example, if two samples per C/A code chip are used (P=2) and K and M are to be 33 and 31 respectively, achieving the full convolution requires performing 31 partial correlations for each shift of the signal shift register, which advances at rate 2×f_(o). Typically, at least two clock cycles are required to read and write RAMs 110 a and 110 b. Assuming two clock cycles, the minimum clocking rate required to achieve the full convolution is: f _(clk)=2×31×2×f _(o)=2×31×2×1.023 MHz≈127 MHz This rate is easily achievable in modern integrated circuit logic.

It should be noted that the invention could also be used to compute a subset of the full convolution. In this case, fewer than M partial correlations are performed for each shift of the signal shift register. In this case, the total range of delays will be less than the P×1023 making up a full convolution. In particular if M₂ partial correlations are performed, then M₂ times K times P delay values are generated. The clocking rate to the processor is reduced by the ratio of M₂ to M. Furthermore, the size of the RAMs is reduced by this ratio as well. Thus, this alternative may be useful in systems that do not have the computation or memory resources to process the full convolution.

Other choices for K and M result allows further design tradeoffs to be made, however, since the prime factors of 1023 are 3, 11, and 31, the choices for K and M are limited. Reducing K is desirable since this reduces the size of the shift registers 401 a and 401 b and the complexity of the vector multipliers 402 a and 402 b, but requires a larger M and therefore a large clocking rate. The choices for K are 3, 11, 31, 33, 93. These choices would require clocking rates of 1.39 GHz, 380 MHz, 135 MHz, 127 MHz, and 45 MHz respectively (always assuming P=2 and 2 clock cycles per partial correlation.) Based on the technology available at the time of the demonstration, the K=33 choice was made for one embodiment. With future technologies, the choice of K=11 and a clock rate of 380 MHz may become viable and would result in a further reduction of the logic complexity. Thus, the architecture has the desirable attribute of supporting optimized tradeoffs between speed and logic complexity.

The sequencing of code segments is controlled by control logic 414. This control logic also identifies the correct addresses for the RAMs 110 a, 110 b and 113. As will be discussed below, the partial correlations are generated in a non-sequential order, thus the generation of RAM addresses is non-trivial.

The operation of the circuits of FIG. 4 can also be understood by reference to the flow diagram of FIG. 5. Operation begins at step 501 with pre-loading of the signal shift registers 401 a and 401 b. At this point, convolution processing can begin. At step 502, a code segment is accessed for the particular partial correlation. At step 503, the code segment is extended by the code extender to have P samples per C/A chip. Next, at step 504, the delay index and corresponding RAM addresses are computed. The delay index indicates which point of the full convolution will be updated by the partial correlation. As will be apparent from the example discussed in conjunction with FIG. 7, the delay index jumps around in a non-linear, but deterministic manner. The address computation is a function of the number of signal shifts and the code segment.

At step 505, the partial correlation is computed using the vector multipliers 402 a and 402 b. At step 506, the result is accumulated into the signal RAMs at the location indicated by the delay index. Next at step 507, a check is made to determine whether the processing has reached the end of the coherent integration interval. If not, the method returns back to step 502 a, and repeats for the above steps for the next code segment.

If, at step 507, the check indicates that partial correlations are complete for all code segments (e.g., 31 partial correlations), the method proceeds to step 508. At step 508, the signal registers 401 a and 401 b are shifted by one sample.

The process then moves to step 509, where a check is performed to see if the last shift encountered the end of the coherent integration interval. If not, the process cycles back to the start at step 502. If the check indicates the end of the coherent integration interval, then the method continues to step 510, where the signal magnitude is computed by complex normalizer 111. The result is added using adder 112 and stored in the magnitude RAM 113. Next, at step 511, a check is made to determine if all magnitude accumulations have been performed. If so, the method completes at step 512. If not, processing continues by performing the next partial correlation at step 501.

FIG. 6 and FIG. 7 illustrate, through a simplified example, how the invention utilizes partial correlations to accumulate a full convolution result. For clarity, these diagrams illustrate convolution of a very short length 6 code, as opposed to the length 1023 C/A code of a GPS signal. To further simplify the example, one sample per code chip is used, i.e. P=1. FIG. 6 illustrates convolution through a standard matched filtering approach, and FIG. 7 illustrates the identical convolution through the method of combining of partial correlations. The details of FIG. 7 are helpful in understanding overall operation of the invention. Both methods generate identical convolution results.

FIG. 6 shows the operation of a conventional matched filter for a length 6 signal. Operation begins at a moment in time indicated as shift 0. At this moment, 6 consecutive signal samples comprising an entire cycle of the signal are in the signal shift register 601. Individual samples are labeled with uppercase indices A, B, C, D, E, and F. Code samples for the entire length 6 code are held in reference register 602 and are labeled with lowercase indices a, b, c, d, e, and f. At the time of shift 0, a vector multiplication and add is performed to generate the correlation result for shift 0. Each signal sample is multiplied by a corresponding code sample and the results are summed to yield correlation result 603.

Next, the signal shift register 604 is advanced by one sample, as indicated by shift 1. The signal is periodic, so the new sample introduced at the left side of the register is identical to that shifted out to the right. The shifted contents of the register 604 are now samples with indices F, A, B, C, D, and E. The code is not shifted. The vector multiplication and addition now yields a correlation result 605 for shift 1. This process of shifting continues for 5 additional shifts, at which point all 6 correlation results making up the full convolution are available.

FIG. 7 illustrates how the same convolution result can be obtained through the method of partial correlations. As described, the invention requires that the code be factored into M segments of length K. In the simplified example of FIG. 7, the length 6 code was factored into 3 segments of length 2, i.e. K=2 and M=3. Operation begins at a moment in time indicated at shift 0. At this moment, two signal samples are held in the signal shift register 701. The signal samples are labeled with uppercase indices A and B. The 6 samples of the code are contained in 3 segments each of length 2. The first code segment 702 contains 2 code samples labeled with lowercase indices a and b. The signal is held in place for 3 partial correlation operations, resulting in partial correlation results 703 a, 703 b and 703 c. The first partial correlation result is created by a vector multiplication and addition between the contents of the signal register and the first code segment (segment 1). The second and third results are created by vector multiplications of the signal register with the second and third code segments respectively. Note that the signal register is held in place for a sufficient time for all three-vector multiplications to be performed, and that the code is not shifted during this time, rather different code segments are selected.

The partial correlation results are accumulated into the memory according to the signal paths 705. For example, at shift 0, the partial correlation from the first code segment sums into the correlation result 704. The partial correlation from the second segment sums into the correlation result 706 for shift 2. The partial correlation from the third segment contributes to the correlation result 708 for shift 4.

After three partial correlations, the signal is shifted. At this stage, indicated as shift 1, the signal register contains samples F and A. Again, three partial correlations are generated with the same three code segments as before. The results from these partial correlations contribute to correlation results 710, 712, 714 respectively for shifts 1, 3, and 5. The process continues for 4 additional signal shifts, at which time the full convolution result is available. As can be seen, the operation requires generating a total of 18 partial correlations that contribute to the 6 full results comprising the convolution.

The architecture described by FIG. 7 illustrates two important properties of the invention. First, it is apparent that the full convolution was produced for a length 6 code using only a shift register and vector multiplication and addition unit of length 2. This requires less circuitry than the FIG. 6 where these elements are of length 6. Second, in FIG. 7, the code samples are accessed in fixed segments that are the same for each shift, and each segment is a separate non-overlapping section of the code. Thus, a simple lookup or register scheme can be used to provide the code to the vector multipliers, as will be discussed further in reference to FIG. 8 and FIG. 9. These schemes require less circuitry than other architectures that might, for example, require large blocks of code bits to be made available in a more complex set of permutations. The invention also eliminates the need to provide code generation circuitry.

FIG. 8 shows a block diagram of one embodiment of a code lookup circuit 408. Table 801 contains stored values for all 1023 bits of each of 32 codes, for example in read-only memory (ROM) or hard-wired logic. The table 801 is organized as 32 sub-tables, one for each code. Each sub-table is further organized as M segments of length K where K×M=1023, and K and M are chosen as described previously. Multiplexer 802 selects a particular code based on a select value. The output of multiplexer 802 is a particular sub-table for the desired code. Multiplexer 803 selects a particular segment based on a segment select value between 1 and M. The output of 803 is a particular code segment 804, of length K, which contains code bits provided to code extender 409.

It should be noted that multiplexer 803 must be high speed in order to allow the code segment to be changed each partial correlation, i.e. every two clock cycles. For this reason, it is necessary that all code bits be pre-stored in table 801, as opposed to being generated on the fly in the traditional manner of a code generator.

The circuits of FIG. 8 are intended to be illustrative. In practice, there are many different circuit designs that are functionally equivalent. In particular, the process of logic synthesis used in modern ASIC design will lead to a certain pattern of gates that achieves a behavior equivalent to that described above but not necessarily using multiplexers in the manner described.

FIG. 9 shows a block diagram of an alternate embodiment of a code lookup circuit 408. The 1023 code bits corresponding to a particular code are held in 1023 dual-directional shift registers 901, organized as M rows of length K. The shift registers operate in two modes: a running mode, and a loading mode.

In the running mode, each register 901 is configured to shift its sample to the register above it in the next row, except for the top row of registers that shifts to the bottom row of registers. The shift directions for running mode are indicated by solid arrows within 901. By clocking all the registers, rows of code bits will circulate, such that at any one time the top row contains one of M code segments of length K. This top row of bits is provided to code extender 409. The registers circulate rapidly, so that a different code segment is made available for each partial correlation.

In the loading mode, each register is configured to shift its sample to the register next in its row, except for the last column of registers, which shift to the first column of registers in the row above. The shift directions for loading mode are indicated by dotted arrows within 901. The left-hand lower shift register 904 is connected to code generator 902. The code generator is a traditional code generator, capable of sequentially creating the 1023 code bits of a particular code based on a select value. When the code lookup circuit is configured for a particular code, the registers are placed in the loading mode, and the generator is used to generate the bits of the code, which then clock through the registers. After all bits have been clocked through, the code will reside in the registers as M segments of length K. The circuit is then ready for use in the running mode.

FIG. 10 depicts a block diagram of an alternative embodiment of a GPS receiver 1000 capable of operating in multiple modes of resolution. The GPS receiver 1000 has a convolution processors 1009 that operate either in a standard resolution mode or a high-resolution mode. Moreover, digital signal samples in standard resolution mode are spaced ½ of a C/A code chip apart (i.e., P=2). Digital signal samples in the high-resolution mode are spaced 1/5 of a C/A code chip apart (i.e., P=5). As such, the Code NCO 1008 and the decimation circuit 1007 operate at a plurality of sampling rates. Those skilled in the art can readily devise other values for the sample spacing and understand that the invention can operate in more than two modes of resolution.

The embodiments of FIG. 10 has similar components as those depicted in FIG. 1. Components having the same reference number as those in FIG. 1 operate as described above with respect to FIG. 1. Components such as decimation circuit 1007, Code NCO 1008, convolution processor 1009 and mode selection processor 1002 operate as described below to facilitate the use of a plurality of resolution modes. FIG. 10 further comprises a mode selection processor 1002. The mode selection processor 1002 processes received signals to determine whether the processing channel 1004 should operate in the high or standard resolution mode.

As with the embodiment shown in FIG. 1, FIG. 2 depicts waveforms generated by the components of FIG. 10. Although the waveforms depicted in FIG. 2 are illustrative of operation in standard mode, operation in high-resolution mode would generate waveforms of similar character. Specifically, if P=5 in high-resolution mode, the total number of points in the full convolution would be 5115 rather than 2046. However, as will be described more fully below, only a portion of the convolution is generated in the high-resolution mode.

It should be noted that in standard resolution (i.e., P=2), the least square estimation uses only 4 points over the width of the correlation, as shown by the width 303 of the triangle base in FIG. 3. In the presence of noise, this limits the accuracy of the curve fitting process. Furthermore, in many cases the center of the triangle (i.e., the point of maximum correlation) will reside between the observed correlation values. In this situation, the observed correlation, and hence the observed signal to noise ratio, is significantly lower than the case where the peak of the triangle is close to an observed point. The high-resolution mode improves accuracy and signal to noise ratio by including many, finely spaced points in the least squares estimation process.

Specifically, FIG. 11 shows the details of an accumulated magnitude waveform when the same correlation as shown in FIG. 2 is processed in high-resolution mode. The graph 1100 shows the magnitude of the convolution in the vicinity of a peak 212 ₃ corresponding to the time delay of the signal processed in high-resolution mode. Points on the code chip axis 210 are spaced at an interval equal to the C/A code chip length divided by P, where P is the ratio of the signal-sampling rate to f_(o), the C/A code chipping rate. In the high-resolution example, P=5, so the points are spaced at ⅕ chip intervals, or approximately 200 ns. (This spacing in time corresponds to a range difference of approximately 60 meters). In order to achieve high accuracy pseudorange measurements, the output of the convolution is further processed, typically in the CPU 114.

As with standard resolution processing, there are numerous interpolation techniques that can be used to estimate the true time delay, using discrete correlation values provided by the convolution. One embodiment uses a least squares estimation technique to identify parameters of a signal that best fits the noisy data. The correlation response takes on the form of a raised triangle 1102. The width 1103 of the triangle 1102 is exactly 2 C/A code chips, which corresponds to 11 sample points (for the P=5 case). The height 1104 of the base of the triangle 1102 is the magnitude of the noise in the convolution for time delays not corresponding to the signal. The magnitude of this noise can be estimated from the data or pre-calculated based on design parameters, such as the amplifier noise figure, cable and filter loss, and system temperature. The peak 1105 of the triangle 1102 and the center 1106 are unknowns corresponding to the signal magnitude and time delay. The least squares method can be used to estimate these two parameters so as to fit the noisy data points to a triangle with a particular peak and center.

One benefit of the high-resolution mode over the standard resolution mode is that the raised triangle correlation response is sampled at more than twice as many points. As understood by those skilled in the art, the accuracy of the fitting process depends on the number of values used in the estimation. Furthermore, the ratio of the peak of the triangle to the base of the triangle is increased in high-resolution mode. This indicates an improvement in signal to noise ratio, due in part to correlation points being available close to the point of maximum correlation. Thus, high-resolution mode can be used to reliably identify and measure correlation peaks that may not be properly discernable in standard mode. This can be very advantageous when processing low energy signals, such as those signals received indoors from GPS satellites.

As will be described further with regard to FIG. 12, the two modes of operation are achieved by dynamically changing the values of the parameters P, K, and M to obtain the desired resolution. In one embodiment, P=2 (i.e., two samples per C/A code chip) in standard mode and P=5 (i.e., five samples per C/A code chip) in high-resolution mode. The completed correlation points are spaces at 1/P chips apart, thus it is clear that the larger the value of P, the finer the resolution. As discussed above, K is chosen as a design parameter and is a factor of 1023. For simplicity, the remainder of the discussion focuses on one particular embodiment where P=2 and K=33 in standard mode; and P=5 and K=11 in high-resolution mode.

FIG. 12 illustrates a block diagram of another embodiment of a convolution processor 1009 suitable for operation of the invention in multiple modes of resolution. For simplicity, only the I channel of processing is shown, but it is clear that the Q channel comprises identical processing elements. In the present embodiment, the convolution processor 1009 comprises a shift register 1201, a vector multiplier circuit 1202, an adder 1203, a code extender 1209, and a code lookup table 1208. The code extender 1209 further comprises a standard code extender 1204 and a high-resolution code extender 1205. The I signal from the decimation circuit 1007 is coupled to the shift register 1201. Shift register 1201 is of variable length since the value of P×K changes with regard to standard and high-resolution modes. Specifically, shift register 1201 must hold 66 samples in standard mode and 55 samples in high-resolution mode. Thus, shift-register 1201 comprises 66 elements to support both lengths. In high-resolution mode, the last 11 elements are disabled.

Signals advance through shift register 1201 at the rate of Pf_(o) as timed by the code NCO 1008 for either standard mode or high-resolution mode. The signals remain in place for many clock cycles so that a series of partial correlation operations can be performed. Specifically, a total of M partial correlations are performed, where M=1023/K. For the present example, in standard mode, M=31, and in high-resolution mode, M=93. Each partial correlation consists of a fast vector multiply and add operation between the contents of shift register 1201 and a segment of the code containing P×K code samples. The operation is performed via vector multiplier 1202, which comprises multipliers 1210 and a summer 1212. Similarly to shift register 1201, vector multiplier 1202 is of a variable length to support both standard and high-resolution modes of operation.

The correlation operation consists of multiplying each of the P×K signal samples in shift register 1201 by P×K code samples (formed by extending the code samples with code extender 1209), and summing the results in summer 1212. As discussed above, mathematically, this operation is referred to as the inner product. The results of the vector multiply and add are accumulated by adder 1203 and processed by the convolution results processing circuits 400 in the same manner as discussed above with regard to FIG. 4.

Code lookup table 1208 generates the reference code samples for each partial correlation and is organized to supply code segments for both standard and high-resolution modes. First, the code must be selected from 1 of 32 codes. This selection is constant through the convolution process and is established when the processing channel is configured to correlate for a particular satellite signal. The second index is a segment index between 1 and M. In the present example, the number of samples per segment is 33 in standard mode and 11 in high-resolution mode. To support both modes, the code lookup table 1208 comprises 93 segments 1207 of 11 chips. The 93 segments 1207 are further organized into 3 blocks 1206 a-c of 31 segments each. The output of each group 1206 a-c (an 11 chip segment) is coupled to the code extender 1209.

In standard mode, the output segment of each group 1206 a-c is combined to form a wide segment having 33 chips. Specifically, a segment selection is made between 1 and 31. The segment selection and the code selection are used to multiplex 3 segments 1207 of 11 samples from groups 1206 a-c. The segments 1207 are concatenated to form a 33 sample wide segment, which is the input to the standard code extender 1204. In high-resolution mode, the segment selection runs from 1 to 93. Only one of the segments 1207 is chosen from groups 1206 a-c. The 11 sample segments 1207 are then coupled to the high-resolution code extender 1205.

In standard mode, the standard code extender 1204 is active, which extends the 33 sample wide code segments to 66 samples. In high-resolution mode, the high-resolution code extender 1205 is active, which extends the 11 sample code segments to 55 samples. Although the code extender 1209 is shown as comprising a standard code extender 1204 and a high-resolution code extender 1205, it is understood by those skilled in the art that they could be functionally combined into a single code extender 1209.

Clock rates change between standard and high-resolution modes. For example, in standard mode, as discussed with regard to FIG. 4, a clocking rate of approximately 127 MHz supports performing a full convolution in real time for the case where P, K, and M are 2, 33, and 31 respectively and two clock cycles are needed per RAM cycle. In the present embodiment, the high-resolution mode parameters P, K, and M are 5, 11, and 93 respectively. Thus the clocking rate to generate the full convolution is: f _(clk)=5×93×2×f _(o)=5×93×2×1.023 MHz≈952 MHz Since this rate is difficult to achieve in modern integrated circuit logic, and since the size of the RAMs would grow from 2046 samples to 5115 samples, it may be desirable to generate less than the full convolution when operating in high-resolution mode in order to reduce cost and complexity of the convolution processor 109.

Therefore, in one embodiment, less than the full convolution is computed in high-resolution mode by reducing the number of partial correlations performed for each shift of the input signals. As will be describe below with regard to FIG. 13, the partial correlations are selected so that points of correlation are generated for a specific region of interest within the full convolution. In this alternative embodiment, the clock rate required is: f _(clk)′=5×L×2×f _(o) where L, a number smaller than M, represents the number of partial correlations per input cycle shift. Thus, the total number of correlation points generated is P×K×L. For example, in one embodiment L=12 and P×K×L=660, or about ⅛ of a C/A code epoch. In this example, the clocking rate required is: f _(clk)=5×12×2×1.023 MHz≈123 MHz a value that is commensurate with the clocking rate in standard mode.

Since only a subset of the full convolution is generated, it is necessary to select a portion of interest containing the signal peak. FIG. 13 depicts a flow diagram of a method of operation 1300 of the invention for computing multiple correlation resolutions. The method 1300 begins at step 1302. At step 1304, checks are made to determine whether sufficient external aiding information exists that enables direct use of high-resolution mode. This aiding information could take several forms, including estimated pseudoranges for satellites of interest and an estimate of local clock bias. If the aiding information is sufficiently accurate, the method transitions to high-resolution mode at step 1310. Often times, however, the local clock bias is unknown. For example, estimated pseudoranges may be available from stored ephemeris and a last known receiver position, but, unless the receiver maintains precise timekeeping or is externally synchronized, the local clock bias will be unknown. If there is not sufficient external aiding information, pseudorange measurements are made in standard mode at step 1306. At step 1306, a full convolution is obtained using a standard resolution. After one or more measurements are made in standard mode, the local clock bias is estimated at step 1308. This step optionally includes an estimation of time tag error. The method 1300 then transitions into high-resolution mode at step 1310. At this point, the signal delays can be bounded to a plurality of windows bracketing the correlation peaks at the standard resolution, which is computed at step 1312. After the range windows are computed, the method 1300 makes pseudorange measurements in the high-resolution mode (i.e., using the high resolution correlation peaks) at step 1314. The method 1300 ends at step 1316.

The method 1300 allows the high-resolution mode to be used beneficially notwithstanding the constraint that only a partial convolution is computed. As long as at least one satellite is detected in standard mode, high-resolution mode can be invoked. In high-resolution mode, the sensitivity of the correlation processing is enhanced, which enables additional satellites to be detected. Furthermore, as described above, the accuracy of all measurements is improved in high-resolution mode.

As described above with respect to FIG. 1, the convolution results produced by the convolution processor 109 may be coherently integrated over many milliseconds (i.e., many epochs of the signal). The signal-to-noise ratio of the convolution results is maximized by increasing the length of time over which the convolution results are coherently integrated (“coherent integration period”). Maximizing the signal-to-noise ratio of the convolution results minimizes the “squaring loss” produced by the non-linear magnitude accumulation process. However, as described in detail below, a longer coherent integration period results in a narrower frequency response of the combined correlation and coherent integration process.

FIG. 14 depicts a graph 1400 showing exemplary frequency response waveforms for various coherent integration periods. The graph 1400 includes an axis 1402 representing the deviation of frequency in the received signals from an expected frequency, and an axis 1404 representing the normalized sensitivity of the correlation and coherent integration process. In general, the frequency response is a sinc function having a first null (first zero) at a frequency of 1/T, where T is the coherent integration period. Frequency responses for coherent integration periods of 1 millisecond, 2 milliseconds, and 4 milliseconds are depicted by waveforms 1406, 1408, and 1410, respectively. As is apparent from the waveforms 1406, 1408, and 1410, the frequency response of the correlation and coherent integration process narrows as the coherent integration period is increased.

The frequency of the received signals may deviate from the expected frequency due to: (a) Doppler associated with the satellites, which is typically less than ±4 kHz; (b) Doppler associated with the motion of the receiver 100, which is typically less than several hundred Hz; and (c) frequency errors associated with the reference oscillator of the receiver 100, which can range from hundreds of Hz to tens of kHz, depending on the quality of the reference oscillator employed in the receiver 100. In an assisted GPS system, aiding data may be supplied to the receiver 100 that provides an accurate estimate of the Doppler in the received signal. As such, a-priori knowledge of the Doppler is known, longer coherent integration periods may be used without a loss in sensitivity due to the roll-off of the frequency response. That is, the receiver 100 compensates for the Doppler in the received signal, which results in the signal frequency remaining near the peak of the frequency response.

In some cases, the receiver 100 may not have a-priori knowledge of the Doppler in the received signal. For example, the receiver 100 may be operating in an autonomous mode, where no aiding information is provided to the receiver 100. Uncompensated Doppler in the received signal limits the duration for coherent integration due to the frequency roll-off described above. This is apparent from the waveforms 1406, 1408, and 1410, which show that the sensitivity of the correlation and coherent integration process is substantially reduced as the frequency error increases. For example, given a coherent integration period of 4 ms (the waveform 1408), the sensitivity is reduced by one half when there is a frequency error of approximately 150 Hz. Thus, in order to detect a correlation peak, multiple correlations may be performed at different frequency offsets (“frequency bins”).

FIG. 15 depicts a graph 1500 showing exemplary frequency response waveforms for different frequency bins. The graph 1500 includes an axis 1502 representing the deviation of frequency in the received signals from an expected frequency, and an axis 1504 representing the normalized sensitivity of the correlation and coherent integration process. Frequency responses for frequency bins of 0 Hz, 500 Hz, 1000 Hz, and 1500 Hz are depicted by waveforms 1506, 1508, 1510, and 1512, respectively, where the coherent integration period is 1 millisecond. The frequency bins are selected to cause the frequency responses overlap such that the sensitivity of the correlation and coherent integration process stays above a predetermined threshold. In the present example, the total frequency interval to be searched is 1500 Hz, the frequency bins are spaced at intervals of 500 Hz, and the normalized sensitivity threshold is approximately 0.9. These numerical values are illustrative of the values that may be used for the total frequency interval to be searched, the frequency bin spacing, and the sensitivity threshold.

Referring to FIGS. 14 and 15, it is apparent that an increase in the coherent integration period requires a search over more frequency bins in order to detect a correlation peak in the received signal. As described above, a longer coherent integration period narrows the frequency response of the correlation and coherent integration process. A narrower frequency response in turn results in narrower intervals between frequency bins in order to maintain a desired sensitivity threshold. Finally, if more frequency bins must be searched, the total time for detecting a correlation peak is increased.

In another embodiment of the invention, the number of frequency bins to be searched in order to detect a correlation peak may be reduced by selecting a coherent integration period of less than one millisecond (i.e., less than one epoch of the received signal). Returning to FIG. 14, a waveform 1412 depicts a frequency response of the correlation and coherent integration process for a coherent integration period of 5/31 of a millisecond. The frequency response corresponding to a coherent integration period of 5/31 of a millisecond is broadened by a factor of about six with respect to the frequency response corresponding to a coherent integration period of 1 millisecond. As shown in FIG. 15, given a desired normalized sensitivity threshold of approximately 0.9 and a total frequency search interval of 1500 Hz, only one frequency bin must be searched when a coherent integration period of 5/31 of a millisecond is selected (the waveform 1412). This is in contrast to the four frequency bins that are required when a coherent integration period of 1 millisecond is selected (the waveforms 1506-1512).

In general, any “sub-epoch” (i.e., less than 1 millisecond) coherent integration period may be employed using one or more frequency search bins. Employing a sub-epoch coherent integration period, however, reduces the processing gain prior to the magnitude accumulation operation (i.e., non-coherent integration). That is, the “squaring loss” during the magnitude accumulation operation is increased. To compensate for this increased squaring loss, additional magnitude accumulations may be performed (i.e., the non-coherent integration period may be increased). As described above, non-coherent integration is not affected by phase variations due to frequency error. As such, non-coherent integration does not affect the frequency response of the correlation and coherent integration process. Despite the additional non-coherent integration time, by employing a sub-epoch coherent integration period, the invention achieves faster search times when compared to coherent integration periods of 1 ms or more. The benefit of searching of less frequency bins outweighs the increase in the non-coherent integration period. In addition, by searching less frequency bins, the invention requires less CPU interaction to manage the frequency searching process.

Over long integration times, there is an additional effect that further degrades the correlation response. Specifically, due to the Doppler effect, the signal “stretches” or “contracts” in time. For example, a Doppler error of 2 μs/s (2 ppm), which results in approximately 3 Khz of carrier shift, also represents a time shift of two chips over a period of one second. This time shift effect causes a “smearing” of the correlation peak, since the correlation peaks at later time periods will not line up with those at earlier time periods. As long as this smearing is less than a fraction of a chip it will not significantly degrade the ability of the receiver to detect the signal peak. For example, over 100 milliseconds, a Doppler error of 2 μs/s causes smearing of ⅕th of a chip only. This is acceptable for the purposes of the current invention since, as described above, a secondary higher-resolution correlation may be performed for the purposes of finely resolving the peak location.

The process for correlating a digital signal with a pseudorandom reference code using sub-epoch coherent integration period may be understood with renewed reference to FIG. 5. As described above, a check is made at step 509 to determine if the end of a coherent integration period has been reached. In accordance with one or more aspects of the invention, the coherent integration period may be selected to terminate before an entire repetitive period of the signal is processed. In general, the coherent integration period may be selected to terminate after M′×P×K signal samples have been shifted right at step 508, where M′<M. For example, if M′=5, P=2, and K=31, then 330 signal samples (115 chips) are processed for each coherent integration period. This is in contrast to coherent integration periods of one or more milliseconds, where 2046 or more samples (1023 or more chips, where P=2) are processed for each coherent integration period. At the end of the coherent integration period, the signal energy (or magnitude) is computed at step 510 and the process proceeds substantially as described above.

In some cases, it may be desirable to begin processing the received signals using a sub-epoch coherent integration period and then transition to processing the received signals using a coherent integration period of one or more milliseconds. However, absent a-priori knowledge of the Doppler in the received signals, the frequency error must be estimated so that the correlation may be properly centered.

FIG. 16 depicts a flow diagram showing an embodiment of a process 1600 for estimating the frequency error in the received signals in accordance with one or more aspects of the invention. The process 1600 begins at step 1602, where correlation is performed using a sub-epoch coherent integration period. At step 1604, a check is performed to determine if an energy spike (i.e., correlation peak) has been detected in the convolution results. If not, the process 1600 returns to step 1602. If an energy spike has been detected, the process 1600 proceeds to step 1606, where a first signal delay is estimated using the position of the detected energy spike. The process of determining signal delay is described above with respect to FIG. 3.

At step 1608, the correlation process is continued using the sub-epoch coherent integration period and a second signal delay is estimated at a later time. At step 1610, Doppler in the received signal is computed using a change in delay between the first signal delay and the second signal delay. The change in delay over time is proportional to the rate of change of the pseudorange (“pseudorange rate”). The pseudorange rate is in turn proportional to the Doppler in the received signal. The estimated Doppler may be used to center the correlation. Thus, at step 1612, the correlation process is performed with a longer coherent integration period (e.g., a coherent integration period of several milliseconds) using the estimated Doppler to center the correlation.

In a conventional receiver, it is necessary to establish a coherent lock on the received signal using, for example, a frequency or phase lock loop. The frequency or phase lock loop, once locked, provides an estimate of the Doppler in the received signal. Using such a coherent locking mechanism, however, may result in a lock to a sidelobe of the received signal, rather than the received signal. Second, a coherent locking process takes time and requires a stable signal. The estimation of Doppler using a computation of pseudorange rate, as performed by the process 1600 of the invention, is more robust than the coherent locking process. Since there is no coherent processing in the process 1600, a stable signal is not required and locking on a sidelobe of the received signal is not a concern.

While the foregoing is directed to illustrative embodiments of the present invention, other and further embodiments of the invention may be devised without departing from the basic scope thereof, and the scope thereof is determined by the claims that follow. 

1. A method of computing a correlation between a pseudorandom reference code and a satellite signal, the method comprising: (a) receiving a satellite signal having a repeating code modulated thereon; (b) correlating less than an entire length of a pseudorandom reference code with a portion of the satellite signal to produce a partial correlation; and (c) forming values representative of a magnitude or a power of the partial correlation produced by correlating less than an entire length of the pseudorandom reference code with the portion of the satellite signal to produce an energy signal, wherein the magnitude is the square root of the sum of squared in-phase and quadrature partial correlations; (d) repeating steps (b) and (c) to produce a plurality of energy signals; and (e) summing the plurality of energy signals as each energy signal is produced.
 2. The method of claim 1, further comprising: generating the code segments from a lookup table by selecting one of a fixed number of non-overlapping segments of less than the entire length of the pseudorandom code.
 3. The method of claim 1, wherein the repeating code is a C/A code of a global positioning system.
 4. The method of claim 3, wherein step e comprises: multiplying each sample in the portion of the C/A code with a respective chip of the selected code segment; and summing each multiplication result with other multiplication results to produce the inner product.
 5. The method of claim 1, wherein the period of the repeating code is 1 millisecond.
 6. The method of claim 1, further comprising: dividing the satellite signal into in-phase and quadrature components; and separately performing step (b) on the in-phase and quadrature components.
 7. Apparatus for computing a correlation between a pseudorandom reference code and a satellite signal comprising: a satellite signal receiver for receiving a satellite signal having a repeating code modulated thereon; a correlator for correlating less than an entire length of a pseudorandom reference code with a portion of the satellite signal to produce a partial correlation; and a circuit for forming values representative of a magnitude or a power of the partial correlation produced by correlating less than the entire length of the pseudorandom reference code with the portion of the satellite signal, wherein the magnitude is the square root of the sum of squared in-phase and quadrature partial correlations; wherein the utilization of the correlator to produce a plurality of energy signals is repeated; and a summer for summing the plurality of energy signals as each energy signal is produced.
 8. The apparatus of claim 7 wherein the code generator further comprises: a lookup table for storing and selecting one of a fixed number of non-overlapping segments of less than the entire length of the pseudorandom code.
 9. The apparatus of claim 7, wherein the repeating code is a C/A code of a global positioning system.
 10. The apparatus of claim 9 the vector multiplier comprises: a multiplier for multiplying each sample in the portion of the C/A code with a respective chip of the selected code segment; and a summer for summing each multiplication result with other multiplication results to produce the inner product.
 11. The apparatus of claim 7, wherein the period of the repeating code is 1 millisecond.
 12. An apparatus, said apparatus comprising: a circuit, said circuit comprising: (a) a satellite signal receiver for receiving a satellite signal having a repeating code modulated thereon; (b) a correlator for correlating less than an entire length of a pseudorandom reference code with a portion of the satellite signal to produce a partial correlation; and wherein the circuit is operable to: (c) for values representative of a magnitude or a power of the partial correlation produced by correlating less than an entire length of the pseudorandom reference code with the portion of the satellite signal to produce an energy signal, wherein the magnitude is the square root of the sum of squared in-phase and quadrature partial correlations; (d) cause repetition of correlating less than en entire length of a pseudorandom reference code with a portion of the satellite signal to produce a partial correlation and (c) to produce a plurality of energy signals; and (e) sum the plurality of energy signals as each energy signal is produced.
 13. The apparatus of claim 12, wherein the circuit is operable to select based on a lookup table, one of a fixed number of non-overlapping segments of less than the entire length of the pseudorandom code.
 14. The apparatus of claim 12, wherein the repeating code is a C/A code of a global positioning system.
 15. The apparatus of claim 14, wherein the circuit is operable to: multiply each sample in the portion of the C/A code with a respective chip of the selected code segment; and sum each multiplication result with other multiplication results to produce the inner product.
 16. The apparatus of claim 12, wherein the period of the repeating code is 1 millisecond.
 17. The apparatus of claim 12, wherein: the circuit is operable to divide the satellite signal into in-phase and quadrature components; and the correlator performs the correlating on the in-phase and quadrature components.
 18. The method of claim 1, wherein less than the entire length of a pseudorandom code is ¼or less of the pseudorandom code.
 19. The method of claim 18, wherein less than the entire length of a pseudorandom code is 1/16or less of the pseudorandom code.
 20. The apparatus of claim 7, wherein less than the entire length of a pseudorandom code is ¼or less of the pseudorandom code.
 21. apparatus of claim 20, wherein less than the entire length of a pseudorandom code is 1/16or less of the pseudorandom code. 